Apparatus and method for dispensing small quantities of particles

ABSTRACT

There is disclosed an apparatus and method which is capable of dispensing very small (typically less than 5 mg) quantities of particles to a high accuracy in a repeatable way and without undue wastage. Also, the need for advanced particle formulation is reduced. The apparatus comprises a closed loop control system which uses an electromechanical actuator to deliver impact energy to a supply of particles initially held on a sieve in a hopper. The impact energy causes a small number of particles to fall through the sieve and onto a weight measuring balance. The weight obtained is scrutinised by a processor to see if further actuations are required. In preferred embodiments, the energy of actuation is varied in accordance with the rate of dispensation calculated by the processor. Also, a correction amount can be obtained to take account of the fact that the balance can take a considerable amount of time to settle to its final value.

CROSS-REFERENCES

This application is a continuation of U.S. patent application Ser. No.10/129,463 filed Dec. 3, 2002 which is a 371 National Phase applicationof International Application Serial No. PCT/GB00/04220 filed Nov. 3,2000 which claims priority to United Kingdom Application Serial No.9926335.2 filed Nov. 5, 1999 which are incorporated herein by referencein their entirety and to which applications we claim priority under 35USC §§119 and 120.

The present invention relates to devices and methods for dispensingparticles by mass, in particular, devices which are capable ofdispensing very small amounts (typically less than 5 mg of particles)accurately and reproducibly. The device can also be used to dispensegreater weights accurately, e.g. 100 mg.

This invention is applicable to many types of particle dispensation.Particularly, this invention is applicable to pharmaceutical particledispensing applications such as the filling, with a predetermined doseof particles, of dry powder inhalers, of capsules and of drug cassettesfor use in gas propelled injection systems.

In U.S. Pat. No. 5,630,796, a method and device for accelerating drugparticles through the skin, mucosal surfaces and other layers wasdescribed. This device causes small particles to be entrained in a veryhigh speed gas, accelerating them with sufficient force to penetrate theskin. The particles may constitute powdered drug compounds andcompositions or genetic material which may be attached to carrierparticles (such as gold). Prior to actuation of the device, theparticles are retained between two rupturable diaphragms. When thedevice is actuated and the gas in the gas reservoir is released, thediaphragms rupture and the particles are entrained in the gas flow.Preferably, the two rupturable diaphragms are constituted in the form ofa removable and self-contained drug cassette. This allows the samedevice to be used more than once by simply replacing the cassette eachtime the device is used. It also allows the device to be suppliedseparately to the particles with the choice of which particle toaccelerate being made after manufacturing.

For some applications, the quantity of particles initially contained inthe cassette is required to be tightly controlled. Whilst some drugs,such as Lidocaine are not very dose specific, other drugs such asinsulin are required to be administered in precisely controlled doses.Also, some drugs are extremely potent in their pure form meaning thatvery small amounts should be used. Whilst this potency can be reduced bychanging the formulation of the drug, this results in an increase inoverall expense since an extra formulation step where the pure drug ismixed with an excipient is required. Further, formulation difficultiescan lead to an undesirable delay in bringing the drug product to themarket.

Also, some drugs and vaccines are very expensive meaning that theminimum amount to give the required effect should be used for economicreasons. For example, DNA coated gold particles are expensive and sometherapeutic compounds can cost tens of thousands of dollars per gram.

As can be imagined, it is often essential that cassettes are accuratelyand reproducibly loaded with known quantities of particles for safetyreasons. An overdose of some drugs may have disastrous consequenceswhereas an underdose may result in the therapeutic agent not having thedesired effect with equally undesirable consequences.

Furthermore, it is advantageous if cassettes are dosed quickly so that alarge throughput of loaded cassettes may be produced in a given time. Itis further preferred that any apparatus used meets the requirements ofcleanliness associated with pharmaceutical production.

With all this in mind, the present invention addresses the problem thatit has traditionally been very difficult to dose very small quantitiesof particles in an accurate and repeatable way, and without unduewastage. Also, previous dosing methods have not been very tolerant toinhomogeneity in the formulation, shape and size of the particles beingused. Pharmaceuticals have conventionally been dosed using volumetricmethods, which require precise control of process parameters when it isrequired to dose a specific mass of particles.

There are several methods known which might be used to dose smallquantities of particles.

Firstly, a vacuum method is known which will be described with referenceto FIG. 1. Here, a small capillary tube 11 having a plunger 12 of knownswept volume is placed in a supply of particles 13 with the plungerfully extended, i.e. flush with the end of the capillary tube—see FIG. 1a. The plunger is then retracted a certain distance (see FIG. 1 b) andthe particles are sucked into the space left by the plunger in thecapillary tube (see FIG. 1 c). Later, the plunger is extended to pushthe particles from the capillary tube into the cassette or otherreceptacle to be filled see FIG. 1 d. This method suffers from thedisadvantage that although the volume of particles obtained may be quitewell controlled, the actual mass of particles is dependant on thedensity at the time and air pockets and other anomalies may reduce thetotal mass delivered. Further, the pushing action of the plunger impartsforces on the particles which may damage them, especially if they arefragile drug particles. This method suffers from the further problemthat free flowing drug particles are required for accurate dosing. Thus,a drug particle formulation must be developed which results in a freeflowing powder. If the powder is not free flowing, inaccurate dosing canoccur.

A second method (not shown) involves the application of electrostaticprinting technology to particle dispensation, i.e. usingelectrostatically charged particles which are manipulated by means ofelectric fields. This method suffers from the disadvantage that theparticles must be electrostatically charged (which may be undesirable)and that the electronic circuitry required to manipulate the correctnumber of particles onto a surface or into a container is complicatedand expensive. Also, it is very difficult to control the electrostaticfields so that they are not adversely influenced by outsideinterference. A further problem is that it is necessary to charge theparticles consistently and so changes in particle shape and size must beavoided. Differences in particle size have a drastic effect on therelative particle charge achievable. This creates an added formulationburden.

A third method, shown in FIG. 2, known as “doctoring” involvescompacting particles into a receptacle of known volume (see FIG. 2 a)and then using a knife or other sharp blade to remove any excessparticles lying above the top edges of the receptacle—see FIGS. 2 b and2 c. As can be seen, a receptacle 21 is packed with particles 22 untilit overflows. A blade 23 is used to remove the excess particles, abovethe top edge of the receptacle 21, leaving a standard volume ofparticles 24. This method is undesirable because it places severe forceson the particles, not only during the compaction process but also whenthe blade is used to shear off the top layer of particles. This methodalso suffers from the problem that a lot of effort must be put into theformulation of the drug particles so that they are free flowing andhomogeneous. Also, this method is not really suitable for small scaleapplications where less than 5 mg of particles are required to bedispensed accurately.

The present invention is an alternative to the above-mentionedtechniques. It has been found to accurately dispense small numbers ofparticles in a repeatable way, with very little particle wastage. Also,the method does not require undue effort to be put into the formulationof the drug particles. Virtually any particle, regardless ofcomposition, and of any shape and size, can be dosed according to thepresent invention. Thus, the conventional effort put into obtaining ahomogeneous and free flowing formulation of drug particles is obviated.In other words, the present invention allows pure or poorly formulateddrug particles to be dosed accurately.

According to a first aspect of the present invention, there is providedapparatus for dispensing particles, comprising:

a particle retainer for retaining a supply of the particles to bedispensed, said particle retainer having a plurality of apertures fordispensing therethrough of said particles;

a particle release actuator for causing, in response to an actuationsignal, some of said supply of particles to be dispensed from saidparticle retainer through said apertures; and

a weight measuring device for measuring the apparent weight of particlesdispensed from said particle retainer and for outputting a signalrepresenting the measured apparent weight.

The plurality of apertures serves to retain the particles, even thoughthe apertures have an average size larger than the average particlesize. When the particle retainer is mechanically agitated by theparticle release actuator, the particles are dislodged and pass throughthe apertures. The apertures are small enough so that they become“clogged”with particles in the steady state and there are a sufficientamount to ensure an acceptable number of particles are dispensed aftereach actuation. The equipment therefore provides an accurate andrepeatable dispensing mechanism capable of dispensing very small numbersof particles.

The speed of operation can be improved by adding a correction value tothe measured apparent weight to account for the effects ofnon-instantaneous working of the weight measuring device.

Accordingly, a second aspect of the present invention provides apparatusfor dispensing particles, comprising:

a particle retainer for retaining a supply of the particles to bedispensed;

a particle release actuator for causing, in response to an actuationsignal, some of said supply of particles to be dispensed from saidparticle retainer;

a weight measuring device for measuring the apparent weight of particlesdispensed from said particle retainer and for outputting a signalrepresenting the measured apparent weight; and

a processor operatively connected to said particle release actuator andarranged to output said actuation signal thereto and operativelyconnected to said weight measuring device and arranged to receive saidmeasured apparent weight signal therefrom, said processor being arrangedto estimate the actual weight of particles dispensed by adding acorrection value to said measured apparent weight.

The first aspect of the invention, like the second aspect, may utilise aprocessor which supplies an output actuation signal to the particlerelease actuator and receives a measured apparent weight signal from theweight measuring device. A number of preferable features are associatedwith both the first and second aspects of the present invention.Accordingly, the processor of both the first and second aspects may bearranged to provide an actuation signal that has a characteristiccorresponding to the amount of particles desired to be dispensed fromthe particle retainer. Thus, the number of particles dispensed aftereach actuation of the particle release actuator may be controlled bymodulating the signal fed to the particle release actuator. Thismodulation may take the form of varying the amplitude, frequency orpulse width of a signal for example.

The apparatus of the first or second embodiments may also be arranged tocalculate the apparent rate at which particles are being dispensed ontothe weight measuring device. This apparent rate may be used to calculatea correction for estimating the actual weight of particles on the weightmeasuring device at any particular time or additionally (oralternatively) it may be used to control the energy of actuation suchthat a target dispense rate is achieved.

The processor of both the first and second aspects may calculate thecorrection value by incrementing the correction value by a storedstandard weight value for each time that the particle release actuatoris actuated within a defined time period. Thus, an actual weight valuemay be estimated which takes account of recent actuations that have notbeen fully registered by the weight measuring device. For example, ifthe weight measuring device is modelled as having a delay of one second,the correction value is incremented by the stored standard weight valuefor every actuation that occurred within the last second. Preferably,the stored standard weight values are multiplied by a multiplicationfactor and the correction value is incremented by a multiplied standardweight, the amount of multiplication generally reducing in respect ofactuations more distant in the past.

The value used as the stored standard weight increment can be updatedafter each complete dispense cycle by calculating the average actualmass delivered per actuation during the last dispense cycle.

During a dispense cycle, the processor can be arranged to compare eitherthe measured apparent weight or the estimated actual dispensed weightwith a pre-determined weight of particles so as to decide whetherfurther dispensation of particles is necessary or whether the cycle canbe stopped, the correct mass of particles having been dispensed. Thepredetermined weight of particles is preferably represented as thedesired weight of particles to be dispensed minus a tolerance weight.This reduces the likelihood of overfilling.

The apparatus of the first or second aspects may be arranged to track atarget dispense rate by increasing or decreasing the energy of actuationwhen the measured dispense rate is lower or higher than a pre-determineddesired rate value respectively. Alternatively, the rate of dispensingmay be reduced by pausing for a pre-determined period of time afteractuating so that the time between taking weight measurements isincreased, resulting in a decrease in the observed dispense rate.

It is preferable to initially use a relatively high target dispense rateand then change to a relatively lower target dispense rate as thedesired weight of particles is approached. This reduces the likelihoodof overshooting the desired weight of particles.

A preferable construction of the apparatus according to both the firstand second aspects of the invention utilises a hopper having apertureswhich are provided by a sieve across the cross-section of the hopper.For pharmaceutical applications, both the hopper and sieve arepreferably made of 316 stainless steel, although a one piece plasticsconfiguration is also useful.

The apertures are preferably holes having a diameter (or other relevantdimension) of from 50 to 800 μm, more preferably 80 to 400 μm, even morepreferably 100 to 250 μm or more preferably still 180 to 250 μm.

The particle release actuator is preferably an electromechanicalactuator such as an solenoid which is arranged to deliver asubstantially horizontal impact energy to the side of the particleretainer. This is preferable to delivering impact energy to the top ofthe retainer since access to the retainer is not hindered and tappingthe side of the container is found to provide more consistent resultsthan tapping the top.

To protect against airflows or pressure differences, an enclosure ispreferably provided for covering at least the weight measuring deviceand the particle retainer, and possibly also the particle releaseactuator.

Conventional vibration techniques suffer from the problem that they aredifficult to control because the particle dispense rate is not linearlyrelated to the frequency or amplitude of vibration. Once the particlesare flowing, a flow limit is established beyond which higher dispenserates are difficult to achieve with precision. The present inventionovercomes this by providing that the particles do not flow so as toreach the flow limit. The use of a particle release actuator means thata substantially discrete impulse of force can be applied to the particleretainer so that particles are dislodged momentarily. This method ofdispensing can be used to provide very accurate dispensing down to verylow weights and is also more controllable than continuous vibrationtechniques because the mass of particles dispensed after each actuationis more linearly related to the force of actuation.

The present invention also has the advantage that there are norelatively moving parts associated with those parts in contact with theparticles. Previous techniques have used pins or screws which move toregulate particle flow. These can trap particles causing damage. Thepresent invention also avoids the problem of mechanical damage which canoccur when parts which move relative to one another are used and iseasier to clean and maintain.

According to a third aspect of the present invention, there is provideda method of accurately dispensing particles, comprising the steps of:

retaining a supply of particles to be dispensed;

causing some of said supply of particles to be dispensed through aplurality of apertures from their retained position to a position wheretheir weight can be measured;

measuring the apparent weight of said dispensed particles; and

utilising said measured apparent weight to control particledispensation.

The method of the third aspect of the invention allows accurate andrepeatable dispensing of a small number of particles. Further accuracycan be obtained by estimating the actual weight of particles dispensedby adding a correction value to the measured apparent weight. Thisalleviates the effects of delays in obtaining a correct weightmeasurement, which are primarily due to delays originating from theweight measuring device, but also from the electronics and due to thetime it takes for the particles to fall from the particle retainer tothe cassette.

According to a fourth aspect of the present invention, there is provideda method of accurately dispensing particles, comprising the steps of:

retaining a supply of particles to be dispensed;

causing some of said supply of particles to be dispensed from theirretained position to a position where their weight can be measured;

measuring the apparent weight of said dispensed particles;

estimating the actual weight of particles dispensed by adding saidmeasured apparent weight to a correction value to thereby reduce theeffects of delays in obtaining a correct weight measurement; and

utilising said measured apparent weight to control particledispensation.

The method of the fourth aspect may be carried out using the apparatusof either the first or second embodiments. Thus, each of the particlesmay be dispensed through one of a plurality of apertures formed in theparticle retainer.

A number of preferable method steps may be carried out in conjunctionwith the methods of either the third or fourth aspect of the invention:

Closed loop control may be obtained by providing that the method stepsare cyclically repeated until a pre-determined desired weight ofparticles has been dispensed within a pre-determined tolerance. Thismitigates against the fact that a different mass of particles may bedispensed following each actuation of the particle release actuator.

The apparent rate at which particles are dispensed is preferablycalculated. This value may be used either to obtain a correction to themeasured apparent weight or to provide feedback in a control loop whichcontrols the rate of particle dispensing (or both).

The correction value used to correct the measured apparent weight can bethe calculated apparent rate which is preferably multiplied by a timeconstant. Alternatively, the correction value may be obtained by addinga stored standard weight for each time that the actuator is actuatedduring a just elapsed time period of some defined length. Each storedstandard weight value used is preferably normalised by multiplying it bya multiplication factor which ranges between 0 and 1. This accounts forthe observation that more correcting needs to be carried out if theactuator was actuated very recently rather than a relatively long timeago. No correction needs to be made in respect of actuations made arelatively long time in the past, since the weight measuring device andother apparatus will have responded fully to these such actuations.

After each dispense cycle, the standard weight value is preferablyupdated so as to more closely correspond to the average weight ofparticles that was delivered in each actuation during the previousdispense cycle.

Closed loop control may be provided by comparing either the measuredapparent weight or the estimated actual weight of dispensed particleswith a pre-determined stored weight and providing a furtheractuation-weighing cycle if the weight falls short of the pre-determinedstored weight. The pre-determined stored weight is preferably a desiredweight of particles to be dispensed minus a tolerance weight.

Dispense rate control may be carried out by causing more or lessparticles to be dispensed than were dispensed in the previousactuation-weigh cycle if the calculated apparent dispense rate is lessor more than a pre-determined desired rate respectively. Alternatively(or additionally), the actual dispense rate can be reduced by haltingthe cycle for a pre-determined or variable period of time. The targetdispense rate can be controlled having regard to the proximity of themeasured apparent weight or estimated actual weight to the desiredparticle weight.

According to a fifth aspect of the present invention, there is provideda particle retainer intended for use in the apparatus of the first orsecond aspect or a particle retainer for retaining a supply of particlesfor use in the method of the third or fourth aspect, said particleretainer comprising:

a hopper;

a sieve across the cross-section of the hopper.

Preferably, the sieve is disposed at the end of the hopper and both areformed of 316 stainless steel. Alternatively, the sieve and hopper maybe formed of plastics material or an electroformed mesh and glass tuberespectively.

The sieve apertures are of a size such that they become clogged with theparticle to be dispensed in a steady state but are readily unclogged fora brief period of time upon the application of external energy to thehopper (which is preferably an elongate duct).

According to a sixth aspect of the present invention, there is provideda processor intended for use as the processor in the apparatus of thefirst or second aspect, or for carrying out some of the method steps ofthe third or fourth aspect, said processor comprising:

signal output means for outputting an output signal of predeterminedcharacteristic to a particle release actuator;

comparison means;

signal input means for supplying the value of an input signal derivedfrom a signal output from a weight measuring device to said comparisonmeans; and

memory means for feeding a predetermined weight value stored therein tosaid comparison means;

said comparison means being arranged to compare said input signal valueto the predetermined weight value and to determine whether said inputsignal is greater than said predetermined weight value.

The processor is preferably a personal computer connectable to a weightmeasuring device and particle release actuator. The personal computer isprogrammed to carry out the appropriate calculations in software. Inparticular, the processor may be programmed to add a correction value tothe signal received from the weight measuring device so as to calculatean estimate of the actual weight of dispensed particles. In fact, theprocessor may, in general, be programmed so as to carry out the variouscalculations described in relation to the methods of the third andfourth aspects of the invention described above.

According to a seventh aspect of the invention, there is provided amanufacturing station for manufacturing a particle cassette comprising:

a collector for collecting an open and empty cassette;

a transporter for moving said open and empty cassette to a position atwhich its weight can be measured;

an apparatus according to the first or second aspect of the inventionfor dispensing particles into said open cassette;

The manufacturing station preferably further comprises a cassetteclosure station which closes a loaded cassette to contain the dispensedparticles and a second transporter for moving the loaded cassettes tothe cassette closure station. The transporter for performing thismovement is preferably the same transporter as is used to move the openand empty cassette. Such a transporter may take the form of a pivotallymounted arm having a locator for locating the cassette at one end, or ofa rotable circular component having such a locator positioned on itscircumference. This locator is advantageously operable to grip andrelease the cassettes. This provides for automatic cassette filling andclosure with minimum human input required.

The cassettes may be fed in on an in-feed track and fed out on anout-feed track. This provides that a “queue” of cassettes may beprovided on the in-feed track such that a machine for manufacturingcassette bodies can be provided in series with the manufacturing stationso as to simply deposit cassettes on an appropriate in-feed track forsubsequent filling.

According to a eighth aspect of the present invention, there is furtherprovided a production line comprising:

a plurality of manufacturing stations according to the seventh aspect ofthe present invention;

an in-feed track for feeding in open and empty cassettes; and

an out-feed track for feeding out closed and loaded cassettes;

wherein said plurality of respective means for moving said cassettes areoperable to take open and empty cassettes from said in-feed track and toplace closed and loaded cassettes onto said out-feed track.

According to a ninth aspect of the present invention, there is provideda particle dispensing station comprising:

a plurality of apparatuses according to the first or second aspect ofthe invention; and

a batch hopper movable between each particle retainer of each respectiveapparatus for refilling each said particle retainer with particles.

According to an tenth aspect of the invention, there is provided amethod of estimating an actual weight of particles dispensed onto aweight measuring device having a non-instantaneous reaction time, themethod comprising:

obtaining a measured apparent weight; and

adding a correction value to said measured apparent weight, saidcorrection value being derived either from a value representing the rateof change of said measured apparent weight or a value obtained bysumming weighted amounts of a value representing the average weightdispensed in one actuation.

The method of the tenth aspect is preferably carried out in software ona computer and is designed to allow an accurate calculation of theactual weight of particles dispensed, even when an accurate weight isnot available from a balance measuring the particle weight. Thissignificantly speeds up a particle dispensing cycle in which particlesare dispensed by performing a number of discrete actuations.

According to an eleventh aspect of the invention, there is provided anestimation function for use with the apparatus of the first or secondaspect, the method of the third or fourth aspect or the processor of thesixth aspect having the form:W _(R) =W(t)+Cwhere W_(R) is the estimated actual weight, W(t) is the current apparentweight and C is a correction value, wherein C has either of these twoforms:

$C = {T\frac{\mathbb{d}W}{\mathbb{d}t}(t)}$ or$C = {\sum\limits_{t = {{now} - t_{p}}}^{t_{now}}\;{{M(t)} \cdot W_{ST}}}$where dW/dt(t) is the current apparent rate of change of weight withtime, T is a time constant, now represents the present time, now-t_(p)represents a time t_(p) ago, M(t) is a multiplication factor and W_(ST)is a standard weight value.

The present invention will be further described by way of non-limitativeexample with reference to the accompanying drawings, in which:

FIGS. 1A-1D are schematic cross-sectional side elevation viewsillustrating a way of dosing particles according to a prior art vacuummethod;

FIGS. 2A-2C are schematic cross-sectional side elevation views showing aprior art method of dosing particles known as “doctoring”;

FIG. 3 is a schematic partially cut away side elevation of apparatuswhich illustrates the general concept of the present invention;

FIG. 4 shows schematically, in partially cut away side elevation and ina simple form, an apparatus according to the present invention;

FIG. 5 is a flow diagram which exemplifies a first embodiment of amethod according to the present invention;

FIG. 6 shows a graph of how the signal outputted by a balance typicallyvaries with time in response to the balance being instantaneously loadedwith a weight W_(R) particles;

FIG. 7 shows a graph of how the signal outputted by a faster-actingbalance typically varies with time in response to a balance beinginstantaneously loaded with a weight W_(R) of particles at time t=0;

FIG. 8 is another flow diagram which exemplifies a second embodiment ofa method according to the present invention;

FIG. 9 is an idealised graph of how the signal outputted by a balancevaries with time in response to the balance being instantaneously loadedwith a mass of particles;

FIG. 10 is a further graph of how the signal outputted by the balanceideally varies with time as the balance is continuously loaded withdiscrete masses of particles;

FIG. 11 shows a flow diagram exemplifying a method according to thethird embodiment of the invention;

FIG. 12 shows a balance response idealised as a delay of t₁;

FIG. 13 shows a graph of how a correction multiplier varies according toa third embodiment of the method of the present invention;

FIG. 14 is a further graph of weight against time which shows how thetarget dispense rate can be varied over time;

FIG. 15 is a further flow diagram which exemplifies a method similar tothe second or third embodiments, but utilising dispense rate control andin which a settled reading is output;

FIG. 16 is yet a further flow diagram which exemplifies a method similarto the first embodiment, but which uses dispense rate control;

FIG. 17 shows, in schematic side elevation, a preferred apparatus foruse in carrying out a method of the present invention;

FIG. 18 shows, in a perspective view from above, three devices accordingto the present invention arranged as a particle dispensing station;

FIG. 19 shows, in partially cut away side elevation, a sample tube andthe batch hopper of the FIG. 18 apparatus;

FIG. 20 shows schematically, in top plan view, a manufacturing device asprovided by the present invention;

FIG. 21 is a partially cut-away sectional view along the line A-A inFIG. 20;

FIG. 22 shows schematically, in a perspective view from above, anexemplary embodiment of the invention for use in a large scaleproduction run;

FIG. 23 is a perspective view of a particle dispensing device inaccordance with the present invention having a removable clamp and apneumatic raising/lowering device;

FIG. 24 is an exploded view of part of FIG. 23;

FIG. 25 is a cross-sectional side-on view of the apparatus shown in FIG.23; and

FIG. 26 is a graph showing how the measured apparent weight andestimated actual weight vary during a typical dispense cycle.

APPARATUS OVERVIEW

An overview of the apparatus according to the invention is shown in FIG.3. As can be seen in this FIGURE, the apparatus has three maincomponents. The first is a particle retainer 31 which serves to retainthe particles 32 within its confines. The particle retainer isoperatively linked to a control means 33 which is able to send signals35 that cause the particle retainer to release some of the particles.The control means is also operatively linked to a weight measuringdevice 34. The weight measuring device is constituted so as to receiveparticles which are released from the particle retainer 31 and tomeasure their accumulated weight This weight measurement is passed tothe control means 33 as a signal 36.

A preferred apparatus is shown in more detail in FIG. 4. The particleretainer 31 is, as shown, constituted by a substantially frusto-conicalhopper having a small diameter at its base (preferably 1-3 mm, but couldbe up to 10 mm). At the lower end of the hopper is a sieve 46, which maybe an electro-formed mesh having holes of the order of 130 μm. The holesize is chosen having regard to the nature of the particles to bedispensed. For example, 130 μm is the value appropriate for dispensingDNA coated gold particles, 250 μm is appropriate for Lidocaine particles(whose diameter is approximately 30 μm) and Alprostadil requires a valueof between 200 and 300 μm. The optimum hole size is typically obtainedhaving regard to the particle size and to other factors such as theflowability of the powder formulation. An empirical trial and error canbe used to fully optimise the hole size for a particular formulation.For pharmaceutical applications, the hopper and sieve are preferablyeach be made of 316 stainless steel and are additionally detachable fromone another to aid in cleaning and disinfecting (if necessary)in-between changing batches. As a further alternative, a one-piecestainless steel or moulded plastics hopper and sieve could be used. Whenplastics are used, the hopper and sieve can be simply disposed ofin-between batches. The diameter of the hopper itself can be anysuitable FIGURE and can be chosen having regard to the mass of particlesto be dispensed. A suitable value for Lidocaine is 10 mm for example.The particles 32 are located in the hopper and, when the hopper is freefrom any external vibration, are able to sit stably in the hopperwithout falling through the mesh, even though the average particle size(nominal diameter) is smaller than the diameter or other relevantdimension of the apertures of the mesh. This is achieved because thesieve apertures are clogged by particles so as to physically retain themwithin the hopper while the apparatus is in the steady state. Theclogging is localised around the sieve vicinity so that the clogging maybe temporarily alleviated by the application to the hopper of anexternal vibration or other movement. The sieve is not clogged to theextent that the particles will not flow through the sieve even on theapplication of external energy. To ensure this, the hopper may besupplied with, or attached to, additional equipment which ensures thatthe particles remain substantially flowable. Such equipment to fluidiseparticles is standard in the art and so explanation here will beomitted. Another possibility is to treat the particles chemically toensure their flowability. Any standard fluidisation technique may beused in practice.

The control means 33 is preferably comprised of an electronic processor,more preferably a personal computer programmed in a language such asVisual BASIC or C++. The processor is able to transmit a signal 35 to aparticle release actuation means 41 which is preferably constituted byan electromechanical actuator such as a solenoid. The solenoid is shownin FIG. 4 as impacting the side of the hopper which has a substantiallyvertical outer surface and this is the preferred arrangement. Analternative arrangement whereby the actuator impacts the top of thehopper has been tried with success but has been found to have twodisadvantages in terms of consistency of results (i.e. repeatability inthe mass of particles dispensed in response to impacts of identicalenergy) and in terms of access to the hopper to refill it.

The processor 33 passes a signal 35 to the actuator 41 that has acharacteristic which corresponds with the impact energy that theactuator will exert upon receipt of the signal. For example, the signalmay have a higher magnitude to achieve a more energetic impact.Preferably, the signal is a square voltage pulse modulated by amplitude.

The weight measuring device 34 may be a standard balance used formeasuring small quantities and may typically have a dynamic range of 60g and an accuracy of 10 μg. For example a Mettler Toledo SAG285 (TM)balance is appropriate. More accurate balances (such as a Sartorius MC5(TM)) may instead be used if the accuracy of the system as a whole isdesired to be improved. Balances with a lower dynamic range, possiblyspecially made balances, may be used if the speed of the system as awhole is desired to be improved. The weight measuring device 34 suppliesa signal 36 to the processor 33 that is a function of (e.g. isproportional to) the weight applied to the balance. The weight measuredwill typically be the sum of the weight of the particles 43 that havealready been dispensed from the particle retainer and the weight of acassette 42 which is placed on the balance 34 in a position where it isable to catch substantially all of the particles 45 leaving the particleretainer 31. FIG. 4 is shown in schematic form only and it is to benoted that in a practical embodiment, steps would be taken to ensurethat no particles 45 are able to leave the sieve 46 and not fall intothe cassette 42. This is generally achieved by positioning the sievewithin the confines of the cassette cavity so that particles would haveto have a component of movement vertically upward in order to escapefrom the cassette.

It is also to be noted that although the word “cassette” encompassescassettes of the type mentioned in U.S. Pat. No. 5,630,796, it isintended that this word also encompasses any form of containmentapparatus. For example, the word cassette also encompasses pockets,cartridges, blisters for dry powder inhalers, cartridges for drugdelivery devices, capsules for oral delivery of drugs etc. In fact, theword cassette is intended to cover anything into which it is desirableto dispense particles. This may include a substrate made up of excipientonto which particles may be dispensed so that a further substrate can beplaced on top to “sandwich” the dispensed particles between twosubstrates of excipient. The complete package can be used as a tabletfor taking orally which would release the dispensed particles only whenthe excipient has been broken down in the patient's stomach. The wordcassette is also intended to cover intermediate holding devices intowhich the particle dose is weighed before being transferred to thedesired location. For example, the particles could be weighed into acassette before being transferred (by tipping or any suitable method)into a blister, substrate or any other receptacle. This has theadvantage of allowing particle transfer into a final unit which issignificantly heavier than the dose of particles or which is too bulkyto be weighed properly (e.g. a tape containing blisters). A furtheradvantage of this arrangement is that it is compatible with a form ofrapid weighing in which several (e.g. ten) cassettes are loadedsimultaneously and a smaller number of these (e.g. three) are emptiedinto a final receptacle in a combination which gives the desired finalweight. An enclosure 44 is advantageously provided to cover the weightmeasuring device and particle retainer so that the system is notinfluenced by draughts or other environmental factors. The enclosurepreferably at least covers the weight measuring device but may also (asis shown in FIG. 4) cover the actuating means 41 and the particleretainer 31.

Initially, the particle retainer 31 is loaded with a supply of particles32 sufficient to fill at least one cassette 42. Preferably, the supplyof particles 32 is enough to fill a plurality of the cassettes, e.g.seventy. The supply of particles 32 initially clogs the sieve 45 so thatthe particles near the sieve are in a position of unstable equilibrium.Any small perturbation of the hopper may serve to upset this conditionof unstable equilibrium and cause some particles to fall through thesieve. When a certain number of particles have fallen, and in theabsence of further perturbation, another position of unstableequilibrium is reached and the sieve again becomes clogged allowing theprocedure to be repeated until the correct dose of particles has beendispensed.

In practice, perturbations to the particle retainer 31 are provided bythe actuator 41 which in the apparatus of FIG. 4 serves to “tap” theparticle retainer 31. This tapping is achieved typically using a squarepulse of voltage of fixed width to drive the actuator.

In this embodiment, the actuator is a solenoid but in general it couldbe represented by any suitable device or system including motors,springs etc. This tap causes a small quantity of the particles to bereleased and to fall into the drug cassette 42 placed on the weightmeasuring device 34. This quantity tends to be proportional to theenergy of tapping although there is some variation either side of theaverage. This can be a problem if an actuation of certain energy causesan unusually large quantity of particles to be dislodged but thisproblem can be ameliorated by providing very low energy tapping duringthe final stages of a dispense cycle so that even an unusually largequantity of dislodged particles for the expended energy does notincrease the total weight of particles dispensed by more than twice theweight tolerance (the tolerance is defined as the weight either side ofthe desired amount, e.g. a tolerance of 10 μg means±10 μg either side ofthe required amount).

In general, a signal 36 from the weight measuring device representingthe weight of the released particles and the weight of the drug cassette(although the weight measuring device may be calibrated (using a tarefunction) not to show the weight of the drug cassette and only to showthe weight of the released particles) is supplied to the processor 33which may perform further calculations using the obtained weightmeasurement. A comparison is then carried out to see if the weight ofparticles dispensed is greater than or equal to a predetermined valuestored in a memory of the processor 33. This predetermined value ispreferably a value representing the desired weight of particles to bedispensed minus the tolerance weight. If the weight of the dispensedparticles is not greater than or equal to the predetermined value,insufficient particles have been dispensed and the processor 33 sends asignal to the actuator 41 to perform another tap on the particleretainer 31, thereby releasing another small amount of particles.Another weight check and comparison is then carried out. This cyclerepeats until the desired particle weight has been reached or exceededwhereupon the process finishes.

The apparatus described may be used to perform closed loop control ofthe dispensed particle weight. The processor 31 makes decisions onwhether or not to actuate the actuator 41 based on the signal 36emanating from the weight measuring device 34. The processor may alsocontrol the amount of impact energy that the actuator 41 transmits tothe particle retainer 31. In this way, an accurately dosed amount ofparticles can be dispensed to the cassette.

The apparatus of the present invention is particularly advantageous fordispensing small quantities of particles by mass. The amount to bedispensed would typically be less than 5 mg, and may preferably be inthe following ranges (listed in order of decreasing preference): 0-4 mg,0-3 mg, 0-2.5 mg; 0-2 mg; 0-1 mg, 0-0.5 mg The above quoted ranges arenot inclusive of the amount 0.

Exemplary embodiments of methods according to aspects of the presentinvention will now be described with reference to FIGS. 5 to 22. Ingeneral, these methods may be performed by the apparatus shown in FIG. 4or 17 but are not limited thereto. Any suitable apparatus may be used inpractice.

First Embodiment of the Method

A method of dosing particles according to first embodiment of thepresent invention is shown schematically by the flow diagram of FIG. 5.

This embodiment represents one of the simpler forms of the invention.Firstly, the processor 33 causes the actuator 41 to exert a controlledtap on the particle retainer 31. The magnitude of the tap may becontrolled by varying a characteristic (such as the frequency ormagnitude of voltage or pulse width of the signal for example) of signal35 and the initial value used may be stored in a memory. The magnitudeof the tap need not be varied however, with the actuator performing astandard tap against the particle retainer each time. The “tap”described herein may also consist of a series of taps of predeterminedmagnitude and duration or indeed may take the form of continuous orintermittent vibration. The tapping causes some of the particles in theparticle retainer to become dislodged from their clogged position and topass through the apertures in the mesh 46, landing on a cassette placedon the balance. The processor then checks the value of signal 36 to seewhat weight of particles was dispensed as a result of the tappingaction. This weight W is then compared with a predetermined desiredweight W_(s) and a decision is made as to whether more taps arerequired. If more taps are required, the cycle repeats until the weightmeasured by the weight measuring device reaches an acceptable amount.

Typically, the predetermined weight value W_(s) stored in the memorywill be slightly less than the desired final weight by a value equal tothe tolerance of the system. For example, if the weight it is desired todispense is 500 μg and the tolerance is −10 μg, the predetermined valueW_(s) would be 490 μg. This is because the system only looks to see ifthe measured weight is equal to or greater than the predeterminedweight. If the predetermined weight is the minimum possible, there isless risk of over-filling the cassette. The system does not allowunder-filling (i.e. filling to less than the predetermined weight) sincethe cycle only stops when a predetermined value is met or exceeded.

In practice, the balance can be programmed to output sampled weightvalues to the processor at regular intervals, e.g. approximately everyquarter of a second using a Mettler SAG285 balance or 10 times a secondusing a Sartorius MC5 balance. Up to 30 times a second is possible usinga specially modified balance. After the processor has caused theactuator to tap the particle retainer, it will take a value available toit from a buffer of recent values obtained from the balance. It is notabsolutely necessary that the value taken is the most recent weightvalue since in practice the weight can vary quite slowly compared to thesampling period meaning that all the values in the buffer (which may,for example, hold 4 values) are roughly similar. It is preferable thatthe value taken is the most recent measurement. In other words, thetapping of the particle retainer 31 and the outputting from the balanceof the weight signal do not need to be carried out in synchronism forthe invention to operate effectively.

This process and apparatus allows extremely accurate dosing of theparticles because it can be arranged (by using a low actuation impactenergy and a small number of apertures) that only a very small number ofparticles leave the hopper after each tap. For example, if only 10 μg ofparticles leave the hopper after each tap, then dosing can be achievedwhich is accurate to within 5 μg of the desired amount. The actualamount of particles that leave after each tap, however, may be 1 μg oreven lower. This depends on the relative particle/sieve size as well asthe energy of actuation.

Second Embodiment of the Method

It has been found in practice that when standard balances are used, acorrect reading is not obtained instantaneously. Although the particles45 fall from the particle retainer 31 very quickly and settle in thedrug cassette 42 after a very short period of time (e.g. less than 0.25seconds), it can take the balance a relatively longer amount of time tosettle down to obtain the correct weight measurement. FIG. 6 shows thestatic impulse response of a Mettler SAG285 balance which is a typicalcurve of how the balance responds to a sudden increase in load appliedat time t=0. The weight of particles applied (at t=0) to the balance isW_(R). In response to this, the output measurement signal of the balancehas a delay where nothing happens followed by an approximatelyexponential approach to the value W_(R) resulting in an S-shaped curve.This S-shaped curve represents the measurement that the balance outputsand therefore also represents the apparent weight of particles on thebalance at any time. This is the “measured apparent weight”. It cantherefore be seen that it can take many seconds for the measuredapparent weight to reach the correct value. The exact shape of thiscurve depends on the design of the balance.

For example, (as shown in FIG. 6) the settling time of the Mettlerbalance is about 4 seconds (meaning that it reaches an accurate stableweight in 4 seconds). If a lot of taps are required, and it is necessaryto wait for 4 seconds between each tap, then the time taken to fill aparticle cassette becomes prohibitively large. This can be addressed tosome-extent by using a balance which settles to a stable weight in asmaller time. For example, the settling curve of a Sartorius MC5 balanceis shown in FIG. 7 and it can be seen from this FIGURE that a stableweight is achieved in about 2.2 seconds. However, the problem ofnon-instantaneous response still exists and the improved method shown inFIG. 8 has been developed to ameliorate this.

This embodiment is based on the observation that the later part of thecurve of FIGS. 6 and 7 is approximated by a simple exponential curve Cof the type shown in FIG. 9. The method of FIG. 8 is based on theapproximation that the exponential curve C shown in FIG. 9 is a goodapproximation of the final part of the real curve shown in FIG. 6. Thecurve of FIG. 9 may be represented by the equation:

$\begin{matrix}{W = {W_{R}\left( {1 - {\mathbb{e}}^{\frac{- t}{T}}} \right)}} & (1)\end{matrix}$where W is the instantaneous weight measurement, W_(R) is the actualweight of particles dropped on the balance, T is a time constantassociated with the balance and t is time. Differentiating this withrespect to time yields:

$\begin{matrix}{\frac{\mathbb{d}W}{\mathbb{d}t} = {\frac{W_{R}}{T}{\mathbb{e}}^{\frac{- t}{T}}}} & (2)\end{matrix}$Substituting the e^(−t) term from (2) to (1) gives:

$\begin{matrix}{W = {W_{R} - {T\frac{\mathbb{d}W}{\mathbb{d}t}}}} & (3)\end{matrix}$

Rearranging gives a value for W_(R) based only on the absolute weightvalue W and gradient dW/dt at any point in time t:

$\begin{matrix}{W_{R} = {{W(t)} + {T\frac{\mathbb{d}W}{\mathbb{d}t}(t)}}} & (4)\end{matrix}$

Thus, the assumption of exponential characteristics makes it possible topredict the final value that the balance will reach from a knowledgeonly of the current value, the current gradient and the time constant Tof the balance. The apparent rate of change of measured weight can beused to correct the measured weight to obtain a value closer to theactual weight.

The method of the second embodiment is similar to the method of thefirst embodiment except that two extra steps are provided after theinitial weighing step as shown in FIG. 8. After a single actuation, theparticles are nearly instantaneously deposited on the balance and thebalance reacts by moving along the curve of FIG. 6 (or FIG. 7) to theactual weight value. The measured apparent weight signal is continuouslymonitored (by sampling at an appropriate rate, e.g. 30 times a secondusing a Sartorius balance) by the processor and the rate at which weightappears to increase (dW/dt) is calculated. dW/dt is therefore theapparent rate at which particles are being dispensed even though theactual weight of particles on the balance remains constant once theyhave been deposited on the balance. The apparent weight does notcorrespond to the actual rate at which particles are being dispensedsince in reality, the particles are dispensed nearly instantaneously.The apparent weight measurement W and rate measurement dW/dt are thenused to estimate what the final settled weight W_(R) of the balance willbe using equation (4) above. For example, if it is known that after onesecond the weight is a particular value and the gradient of theweight-time graph is a particular value, it is possible to determinewhat the weight after 4 seconds (when the balance has settled to itsfinal value) will be.

It is this estimated final value that is then compared to thepredetermined value stored in memory to see if the correct total mass ofparticles has been dispensed. If the correct amount has not yet beendispensed, the particle retainer 31 is tapped again and the process isrepeated. Estimating the dispensed weight in this way allows muchquicker operation of the device since it is no longer necessary to waitwhile the balance settles.

In practice, the apparent dispense rate is calculated using the weightvalues at two points 1 and 2 and the time between taking these weightmeasurements. It is therefore useful that the processor 33 stores in amemory values representing past weight measurements and valuesrepresenting the time at which these measurements were taken. The rateof increase of weight dW/dt may then be calculated by calculating(W₂−W₁/(t₂−t₁). Alternatively, well-known analogue electronic methodsmay be used to differentiate the apparent weight-time curve.

The impulse response of the balance will not in all cases be a trueexponential curve. To account for this, the value chosen for timeconstant T may be varied to provide the best fit.

The choice of coefficient T is preferably obtained empirically and ithas been found that it is usually in the vicinity of one second, beingin the range 0.5 to 2 s, or more preferably 0.8 to 1.2 s.

During the execution of the method, the particle retainer 31 is tappedmany times and the instantaneous weight measurement at any time will ingeneral be made up of many small individual impulse responsesdistributed over time. It is to be understood that, in general, theseresponses will be of different magnitudes since the amount of particleshitting the balance after each tap is not precisely predictable orconstant. A typical balance output signal is shown in FIG. 10. Thedotted lines show the response of the balance to a bundle of particleshitting the balance after each tap. As a working approximation oflinearity, the resulting signal (solid line) is a composite curve madeup of the many smaller impulse responses.

Taking the general point t in FIG. 10 as an example, the weightmeasurement at this point is made up of the impulse responses due tothree taps. The measured weight at point t is therefore:

$\begin{matrix}{{W(t)} = {{W_{1}\left( {1 - {\mathbb{e}}^{\frac{- t}{T}}} \right)} + {W_{2}\left( {1 - {\mathbb{e}}^{\frac{- {({t - t_{2}})}}{T}}} \right)} + {W_{3}\left( {1 - {\mathbb{e}}^{\frac{- {({t - t_{3}})}}{T}}} \right)}}} & (5)\end{matrix}$Where t₂ and t₃ are the points in time where the second and thirdimpulse responses start and W₁, W₂ and W₃ are the final values of eachindividual impulse response. The gradient at point t is given by:

$\begin{matrix}{{\frac{\mathbb{d}W}{\mathbb{d}t}(t)} = {{\frac{W_{1}}{T}{\mathbb{e}}^{\frac{- t}{T}}} + {\frac{W_{2}}{T}{\mathbb{e}}^{\frac{- {({t - t_{2}})}}{T}}} + {\frac{W}{T_{3}}{\mathbb{e}}^{\frac{- {({t - t_{3}})}}{T}}}}} & (6)\end{matrix}$Making the appropriate substitutions leads to:

$\begin{matrix}{{W_{1} + W_{2} + W_{3}} = {{W(t)} + {T\frac{\mathbb{d}W}{\mathbb{d}t}(t)}}} & (7)\end{matrix}$This gives the final output (W₁+W₂+W₃) solely in terms of the presentmeasured value and the present gradient. In other words, equation (4) isstill a good approximation even when more than one tap is affecting thecurrently measured values.

Third Embodiment of the Method

The third embodiment of the method provides an alternative way ofcalculating the correction value which can be added to the measuredapparent weight so as to obtain a more accurate value for the actualweight of particles on the balance 34 at any one time. The method of thethird embodiment has a number of advantages over the method describedabove in relation to the second embodiment. Firstly, the method is moreempirical, and thus takes account of actually observed phenomena. Thus,the method takes more account of the fact that the actual settling curveof a balance is more S-shaped, rather than truly exponential. Secondly,erroneous results can be obtained when calculating the rate of change inthe second embodiment because the actual settling curve is S-shaped,meaning that there are two positions having the same gradient. Thus, thesame correction amount will be obtained at two positions and this amountwill not be correct for both positions. The method of the thirdembodiment does not have this problem. Further, the method of the thirdembodiment allows the dispense cycle to be interrupted and restartedwithout any adverse effect. If the dispense cycle is interrupted whenthe method of the second embodiment is used, an anomalous value for thedispense rate is obtained which can result in inaccurate dispensing.

The flow chart for the third embodiment is shown in FIG. 11. As can beseen, the method is very similar to the method of FIG. 8 except that theapparent dispense rate is not required to work out the correction value.

The third embodiment of the method provides that the correction added tothe measured apparent weight is determined by the recent history of tapscarried out. Thus, it is necessary that the apparatus used is capable ofrecording when in time the particle release actuator is actuated. In asimple form, the response of the balance could be modelled as a simpledelay of time t₁. This response is shown in FIG. 12. As can be seen fromFIG. 12, when a mass W_(R) is applied to the balance, nothing happens tothe output weight measurement until the time t₁, when the correct weightmeasurement is output. If the balance had such a characteristic, thenthe method of the third embodiment would provide that the correctionvalue is equal to the weight W_(R) multiplied by the number ofactuations that occurred in the just elapsed period of time equal to t₁.Thus, if t₁ was equal to one second, and three actuations occurred inthe last one second, then the correction value would be equal to 3W_(R).In this way, actuations which have occurred, but have not beenregistered are taken into account when calculating the actual weight ofparticles on the balance at any one time. The amount W_(R) used in thecorrection calculation is a stored weight which is assumed to be thesame weight that was dispensed by a single actuation. Of course, theactual weight dispensed as a result of any single actuation is unknownuntil it is measured. A small amount of error will therefore beintroduced by assuming that every actuation is of a “standard” weight ofparticles.

The above calculation can be summarised by the following equation:

$\begin{matrix}{C = {\sum\limits_{t = {{now} - t_{p}}}^{t = {now}}\; W_{ST}}} & (8)\end{matrix}$

Where C is the correction weight to be added to the measured apparentweight, now represents the present time, now-t_(p) represents a timet_(p) ago, and W_(ST) is a standard weight value.

The correction value can therefore be seen to be the sum of each tapthat occurred in the time period (now-t_(p)) to (now).

In reality, the balance settling curve is not a pure delay and actuallyhas the form shown in FIG. 6 or 7 for example. To account for this, the“standard” tap weight mentioned above can be subjected to some scalingbefore it is included in the correction value calculation.

As will be evident from FIG. 7, if the actuator has only just performedan actuation, substantially all of the standard weight W_(ST) will needto be added as a correction because the balance will not have reacted tothe actuation yet. However, for actuations more distant in the past,less of the standard weight needs to be added as a correction becausethe balance will have reacted to some degree to the actuation. As mightbe imagined then, a standard weight normalising function can be obtainedby simply flipping the graph of FIG. 7 about a horizontal axis so as toobtain a graph of how big the correction value should be in respect ofactuations made at different times in the past. A linear approximationto such a graph is shown in FIG. 13. Thus, to account for the S-shapedbalance settling curve, a correction multiplier which ranges between 0and 1 is defined. Each standard tap weight which is used to build up thecorrection value is firstly multiplied by the appropriate correctionmultiplier M. The value of the correction multiplier is found from thegraph of FIG. 13. For example, if the actuator was actuated between 0and 0.35 seconds ago, then the correction multiplier M is 1. This meansthat the standard tap weight W_(ST) will be multiplied by 1 resulting inthe whole of the standard tap weight W_(ST) being added to thecorrection value in respect of actuations between 0 and 0.35 secondsago. For actuations made between 0.35 and 1.35 seconds ago, thecorrection multiplier varies linearly between 1 and 0. Thus, anactuation which occurred 0.85 seconds ago would have associated with ita correction multiplier of 0.5 which would mean that half the standardtap weight would be added to the correction value in respect of thisactuation. In this way, actuations which occurred more distantly in thepast are given less waiting than actuations which have only just beencarried out. This can be summarised by the following equation:

$\begin{matrix}{C = {\sum\limits_{t = {{now} - t_{p}}}^{t = {now}}\;{{M(t)} \cdot W_{ST}}}} & (9)\end{matrix}$

M(t) is the multiplication factor graph of FIG. 13 for example.

This method does not suffer from the problem encountered whencalculating the rate of change in the second embodiment when thedispense cycle is abruptly stopped and then started again. Also, themethod does not suffer from the problem that there my be two parts ofthe settling curve having the same gradient but at different weightsbecause the correction amount is determined purely by how long ago anactuation was and how many recent actuations there have been. It is notdetermined by the gradient of a graph which is unrobust and vulnerableto large changes resulting in large inaccuracies.

The method of the third embodiment requires that a “standard” weight isstored in memory and is used as an approximation to the actual weight ofparticles which are dispensed in any given tap. Changing environmentalfactors may dictate that the average actual weight of particlesdispensed in the tap changes with time. To account for this, the stored“standard” weight can be updated at the end of a complete dispense cycleto account for such changes. This updating is carried out in the presentembodiment by dividing the total weight dispensed in the last cycle bythe total number of taps used to dispense this weight in the last cycle.Thus, if the last cycle delivered 500 μg in 50 taps then the stored“standard” weight would be set to 10 μg. This value would then be usedwhen calculating the actual dispensed weight in the next dispense cycle.

It is to be noted that the correction multiplier graph shown in FIG. 13is preferably optimised empirically since it will not always correspondto the static settling curve of a balance flipped about a horizontalaxis. This is because the dynamic settling curve of a balance can varyfrom the measured static settling curve. That is to say, the settlingtime can actually be much less when the balance is being continuouslyloaded with particles than would be observed when the balance is at restand is loaded with an impulse of particles and is left to settle. Thus,once the balance is in a dynamic reading state, the settling time iseffectively reduced. This fact is represented in FIGS. 7 and 13 abovewhere it can be noted that FIG. 13 shows that actuations more than 1.35seconds earlier are not taken into account whereas the static curve ofFIG. 7 indicates that an actuation 1.35 seconds ago would require acorrection multiplier of about 0.4.

Fourth Embodiment of the Method

The fourth embodiment comprises an extra calculation and adjustment tothe operation parameters which can be used in conjunction with any ofthe above described methods of dispensing.

It has been found that the number of particles released by particleretainer 31 bears a relation to the impact energy with which theparticle retainer 31 is tapped by the actuator 41. Thus, tapping harderusually causes more particles to be released and tapping less hardusually causes fewer particles to be released. This fact can beadvantageously used when particle dosing is required to a high accuracybut large doses compared to the tolerance needed are required. Forexample, if a dosing accuracy of 10 μg is required for a dose of 500 μg,then the method of FIG. 5 would require that approximately fifty 10 μgtaps are carried out. This may take an undesirably long amount of time,even when the actual weight is estimated using a correction based on themeasured dispense rate or sum of recent taps as described above in thesecond and third embodiments. Thus, the fourth embodiment provides animproved method whereby harder taps are carried out near the beginningof the dosing process and less forceful taps are carried out near theend (when high accuracy is required).

This is achieved by predetermining a target dispense rate which isintended to correspond to the actual dispense rate achieved at any onetime. FIG. 14 shows a graph of weight against time which shows apreferable configuration of how the target dispense rate changes withtime. As can be seen, the target dispense rate reflects the fact that alarge dispense rate is required early on but a slower dispense rate isrequired as the actual weight dispensed reaches the target amount. Theprocessor checks to see if the measured apparent weight value (or theestimated actual weight value if appropriate) has reached apredetermined value W_(C). If it has, the target dispense rate isreduced to a different, lower, predetermined value as shown in FIG. 14.The ratio of desired amount to W_(C) is usually kept constant and soW_(C) can easily be obtained by multiplying the desired final weight bythis ratio. As previously discussed, the reduction in target dispenserate has the effect of causing the actuator to tap less hard and sodispense fewer particles per unit time.

FIG. 15 shows a flow diagram similar to that of FIG. 8 in which theabove-described feature of the fourth embodiment is combined with themethod of the second embodiment. The main difference is that thecalculated dispense rate (dW/dt) is compared to the target rate and theforce of tapping is adjusted accordingly (by appropriately adjusting thecharacteristic of the signal supplied to the particle release actuator).The calculated dispense rate is compared with minimum and maximum targetdispense rate values (min and max). If the calculated rate is too low,the tap power on the next and subsequent cycles is increased. If thecalculated rate is too high, the tap power on the next and subsequentcycles is reduced. Thus, initially, when a high target rate is set (bysetting high values of max and min), the tap power will be increaseduntil this target rate is achieved. The values of max and min can be setto be identical but in general are different to allow a range ofacceptable target rates at any time.

The choice of value of the target rate is in general determined by theabsolute value of the estimated actual weight so that as the estimatedactual weight increases, the set target rate will drop and the tap powerwill decrease accordingly. This enables accurate dosing to be achievedin a reduced amount of time. Although two target rates are shown in FIG.14, more rates might be used or a constantly adjusting target rate(inversely proportional to estimated actual weight for example) could beused.

While control based on an estimated weight works well in practice, forregulatory reasons it is often necessary to know the exact final weightof particles in the cassette before the cassette is sealed. Thus, afurther step of taking a settled reading is made in this (FIG. 15)embodiment. This step is taken if the comparison based on estimatedweight shows that enough particles have been dispensed. A settledreading is taken by allowing the balance enough time (e.g. 2 or 3seconds) to settle so that a true weight of particles dispensed isobtained. In practice, a number of consecutive samples (e.g. 30 for aSartorius MC5 balance) may be taken from the balance and these may becompared to determine whether as settled reading has been obtained. Forexample, a settled reading can be assumed when the value of each of the30 samples varies by less than some predetermined amount, e.g. 2 μg. Ifthis true settled weight reading falls short of the required amount,then further taps can be given until the correct amount is obtained.Taking a settled reading provides certainty as to the exact mass ofparticles that have been dispensed.

It is to be noted that a settled reading may, and usually will, be takenin the embodiments of FIGS. 5 and 8 as well (this is not shown) and isnot limited to the FIG. 15 embodiment. Equally, the step of talking afinal settled reading may be omitted from the FIG. 15 embodiment if itis not necessary to know the actual final weight of particles dispensedwith high accuracy.

The need to estimate the actual weight based on correcting the measuredapparent weight value is reduced if a fast settling balance is used.Thus, the method of FIG. 16 may be carried out such that the apparentdispense rate is calculated only for the purposes of adjusting the tappower, and not to estimate the actual weight using the apparent dispenserate.

Preferred Embodiment of Apparatus

FIG. 17 shows a particular embodiment of the apparatus which is suitableto carry out any of the above methods. Like reference numerals denotelike parts in FIG. 4. As can be seen, in this embodiment, the actuator41 is spaced apart from the particle retainer 31 by means of a rod 120.This has a practical reason in that the actuator 41 produces electricaland magnetic fields which can interfere with the sensitive components ofthe weight measuring device 34. The rod 120 serves to transmit thehorizontal impact energy created by the actuator 41 to the side of theparticle retainer 31.

Also, in this embodiment, the particle retainer 31 and the actuator 41are supported by means of a pivot 121 and a spring 122. This allows thelower end of the particle retainer to be lifted and lowered so that itmay fit inside the cassette cavity thereby reducing any risks of theparticles failing to enter the cassette. The particle retainer can belifted to allow the full cassette to be replaced by an empty one. Theparticle retainer 31 is mounted on elastomeric supports 123 so that theimpact energy from the actuator is rapidly damped after each tap so thatthere is no further movement on the sieve. The supports 123 also preventthe impact energy being transmitted to the balance.

Further Embodiments of Apparatus

If large numbers of filled cassettes are to be produced then it isdesirable to implement manufacturing systems and production lines whichcan produce such a large number of cassettes with minimal human input.It is further desirable that such systems and production lines arecompatible with the clean room environment in which it is oftenessential to handle drugs and genetic material.

FIG. 18 shows a particle dosing station which comprises three dispensingdevices according to the present invention. Furthermore, there isprovided a batch hopper 130 which is movable along a track 131 so as torefill the particle retainer 31 of the separate devices. In thisembodiment, each particle retainer would carry approximately 30 minutescapacity of particles and the batch hopper 130 is operable to refilleach particle retainer when it is empty. This minimises the opportunityfor stratification in the particle retainer 31. It also allows theparticles to be handled solely by machine so that there is less risk ofcontamination by humans.

The batch hopper shown FIG. 18 is shown in more detail in FIG. 19. Ascan be seen, the particles 140 come prepackaged in a sample tube 141which can be inverted and directly mounted to the batch hopper 130. Thebatch hopper itself could comprise a particle retainer similar to thoseof the dosing devices so that a set dose of particles is dispensed toeach particle retainer on the production line. Of course much lessaccuracy is required and so a much higher target dispense rate can beused.

It is envisaged that the sample tube can be quickly and easily attachedto the batch hopper and would contain enough particles for many hoursproduction. Also, the batch hopper 130 could be made according to anyknown dispensing technology and is not limited to the dispensing methodof the present invention.

FIG. 20 shows a manufacturing station which is capable of taking opencassettes and outputting closed, correctly dosed, cassettes.

This apparatus comprises a means 150 for moving an open cassette 42 ontothe weight measuring device 34 and means for removing the cassette fromthe weight measuring device once the cassette has been filled. Theapparatus also comprises a means 152 for closing the cassette oncefilled. In this embodiment, the means for moving the cassette comprisesa circular ring 150 rotatable about its centre and having cassettelocation means 151 (three in FIG. 20) located around its circumference.FIG. 21 shows a cross-sectional side view along the line A-A in FIG. 20.As can be seen, the location means 151 support the cassette 42 under aflange 181 on the cassette. At the cassette input position the cassette,is moved into one of the location means by the action of a conveyor.When the wheel rotates the cassette is transferred to the dosingposition at which point it is lifted clear of the location means 151 bya raised surface 182 on the pan of the balance 134. The wheel is thenreversed by a small increment thereby leaving the cassette on thebalance with no contact against the location means. After the cassetteis filled, the wheel rotates again and the cassette is transferred tothe cassette output position, where it is firstly sealed, and thenremoved from the wheel by the action of a second conveyor.

Alternatively, the locating means 151 could be operable to grab andrelease a cassette 42 upon signals given to it by a central controller.

This embodiment enables three tasks to be undertaken simultaneously.Whilst one location means is taking a new cassette, another is near acassette being dosed and another is holding a cassette being sealed.

The manufacturing station described has the advantage that the cassettesare closed very shortly after being filled which minimises the risk ofparticle spillage and contamination. Also, it is possible to achieve arapid transfer between removing a full cassette and providing an emptycassette to the balance which minimises the disturbance to the balance.

The manufacturing station of FIG. 20 may be combined with the batchhopper system of FIG. 18 so as to yield the production line shown inFIG. 22. Here, the operator is only required to supply a number of opencassettes 47 to a cassette in-feed track 160 and the cassettes are dosedand closed automatically. The finished product is supplied to anout-feed track 161. Minimal operator input is therefore required.

The cassette in-feed and out-feed tracks 160, 161 could be combined withthe apparatus of FIG. 18 so as to provide a manufacturing station thathas the function of loading cassettes with particles but not necessarilysealing the cassettes. The in-feed track 160 and the out-feed track 161maybe made up of a basic conveyor system which transports the cassettesusing a moving belt. Alternatively, if the cassette configuration ofFIG. 21 is used, the conveyor could consist of two metal tracks whichthe flange 182 of each cassette rests on. The cassettes would then serveto push each other along the track so that no specific motive means isrequired. When the cassettes are not required to be closed at the samemanufacturing station as they are being dosed, the in-feed and out-feedtracks could take a course which simply traverses the balance. A raisedportion on the balance (as has already been described) would then serveto lift the cassette from the track to enable accurate weightmeasurement. Whatever form the conveyor takes, it is advantageouslycontrolled by the same processor as is used to control the dispensingapparatus.

In the apparatus of the present invention, the delivery rate iscontrollable over a wide range by varying the frequency of taps, impactenergy of taps and the aperture size. Any of these parameters may varyin order to provide a device appropriate to the particular type ofparticle being dispensed.

The closed loop system described has the advantage that it is tolerantof material variabilities as well as process condition variabilities. Itovercomes the fact that the delivery per tap is not necessarily precise.

Also, the present invention has the advantage that there is a very lowrisk of damaging the particles. This is particularly advantageous whendispensing DNA coated gold particles. In addition, there are norelatively moving parts to the hardware and so there is less opportunityfor the particles to become trapped and damaged. Also, the simplicity ofthe device makes it compatible with a clean room environment which isoften required when dosing pharmaceutical compounds.

The particle retainer 31 of the present invention could be removable anddisposable so that separate particle retainer could be used fordifferent drugs. This avoids the problems of batch cross over which mayoccur if the same retainer is used with different particle types.

Sometimes, the particles may become compacted in the particle retainer31 leading to lower overall dispense rates and longer dispense times. Toalleviate this, the particle retainer could be double-ended andinvertible with a sieve at each end. At various points in time dictatedby the processor 33, the particle retainer could be inverted through180° so that dispensing continues through the other sieve. This wouldprevent undue compaction of the particles in the retainer and ensuresmooth and speedy dispensation for the whole time particles are left inthe particle retainer. Alternatively, stirring or other disrupting meanscould be used to break down the compaction. Another way to solve thisproblem is to use a standard particle retainer having a closed top, andsequentially invert it twice (ie turn it through 360°). This woulddisrupt the compaction and allow faster dispensation. Disruption of thissort could be carried out regularly, for example, every 10 minutes.Alternatively (or in addition), standard fluidisation techniques couldbe used to limit particle compaction.

Because of the enclosure to isolate the weight measuring device from theeffects of draughts, it has been found that the present inventionoperates satisfactory even in high air movement such as that found inlaminar flow chambers. Thus, the present invention is able to beeffectively used in a laminar flow area when particularly cleanconditions are required.

FIGS. 23 to 25 show a perspective view of a further embodiment of aparticle dispensing device which is similar to that shown in FIG. 17.The hopper 31 is attached to the rod 120 by a clamp 230. As can be seenfrom FIG. 24, the clamp 230 is fastened to the rod by a bolt and engagesa groove in the external surface of the hopper so as to prevent movementin a vertical direction. The hopper 31 sits in a conical hole 242 at oneend of rod 120 and is thereby prevented from moving laterally withrespect to the rod 120. Like in the FIG. 17 embodiment, a solenoidactuator 41 is disposed at the other end of rod 120 so as to impart asubstantially horizontal impulse of force to the rod 120 and thereon tothe hopper 31. The rod 120 is connected to a member 244 by twosuspension arms 240. These arms 240 are designed to be relativelyflexible in the horizontal direction so that the rod 120 is able totranslate horizontally with respect to the member 244. This movement isdamped by damping cylinder 232 connected to one or both of the arms 240and to the member 244. The member 244 is pivoted about pin 121 to a baseplate 246 which is immovable. This construction allows most of thedispensing apparatus comprising the member 244, the cylinder 232, thearms 240, the rod 120, the actuator 41, the clamp 230 and the hopper0.31 to be pivoted about the axis defined by pin 121. This allows thehopper to be moved substantially vertically so as to bring the sieve 46into and out of the cassette 42. The lifting and lowering is achievedautomatically by a pneumatic actuator 234 disposed below base plate 246.The actuator 234 causes a lifting/lowering member 236 to rise and fallsuch that a vertical force is transmitted to member 244 via connectingpin 238. In this way, the member 244 may be pivoted about pin 121 toraise and lower the hopper 31.

As already mentioned, the hopper 31 is connected to rod 120 by a clamp230. This clamp usually ensures that the hopper cannot move relative tothe rod 120. It has been found, however, that beneficial effects can beobtained when the clamp 230 is not used so that the hopper merely sitsin hole 242 and is able to be perturbed vertically. This clamp-freeconfiguration has been found to be particularly effective when it isdesired to dispense particles which tend to adhere to one another or tothe hopper or sieve. For example, agarose beads tend to displaystickiness which often prevents them form being dispensed at all. If theclamp is not used and the hopper 31 is free to move vertically (and/orto rotate) in the aperture 242, agarose beads may be dispensed. Thereason for this is thought to be that the actuator 41 provides ahorizontal force which is converted in part to a vertical force at thehopper side walls, possibly due to the tapered nature of these sidewalls. This vertical force causes the hopper to vibrate vertically,which serves to fluidise the agarose beads, making them easier todispense. This configuration has the further advantage that the hopper31 is free to rotate in the aperture 242 and in general, the hopper 31rotates when the rod 120 is mechanically activated by the actuator 41.These rotations are thought to be due to asymmetries in the components,for example when the plane of the aperture 242 is not preciselyhorizontal. This rotation of the hopper 31 serves to provide that theactuation force is applied from a slightly different direction on eachactuation such that each tap occurs at a different point on the hoppercircumference. This helps to prevent the particles from becomingcompressed or otherwise stuck together.

Experimental Results

FIG. 26 shows a graph having an ordinate of weight in grams and anabscissa of time in seconds. The curve labelled “1” represents thebalance reading obtained during a dispense cycle (i.e. the measuredapparent weight). The curve labelled “2” represents the determinedactual weight, obtained by adding a correction value to the measuredapparent weight. The algorithm used to obtain the correction value wasthat of the third embodiment and dispense rate control was carried out,so that a lower dispense rate was achieved as the target weight of0.00025 g was approached. The diamonds and squares each represent samplemoments and it is to be noted that a sample was taken once after eachtap of the actuator.

Initially, the balance is sluggish in responding to the taps of theactuator as can be seen from the measured apparent weight curve “1”. Atthis time, most of the determined actual weight value is made up of thecorrection value component. For example, after 1 second (and 10 taps ofthe actuator), the balance reads 6 μg but the actual weight of particleson the balance is predicted to be 50 μg. At this time, the correctionvalue is 44 μg. This correction value tends to stay relatively constantif the hopper is tapped at a fairly constant frequency and with constantforce (as with the present experiment). Thus the correction value tendsto be around 50 μg for the first 4 seconds of dispensation. As thetarget weight of 250 μg is approached, the dispense rate controlalgorithm ensures that the actual dispense rate is reduced by tappingless frequently (5 times a second in this case). As a result, the amountof correction required is reduced meaning that the determined actualweight is more accurate. After 6.2 seconds, the algorithm predicts thatthe target weight has been exceeded and the hopper is tapped no longer.Weight measurement samples are then taken at a rate of 30 times persecond. These samples continue to be taken until it is found that thepresent sample and another one taken 1 second ago are different by lessthan some predetermined amount (e.g. 2 μg). In fact, the balance settlesto a relatively constant value after about 8 seconds and after 9seconds, the dispensation is complete, the measured apparent weight “1”now representing the true weight of particles on the balance. This finalreading is stored in a memory and is regarded as the true weight ofparticles that were dispensed.

Experiments to dispense three different powder compounds were conductedusing the correction algorithm of the third embodiment together with thetarget dispense rate control of the fourth embodiment. A Sartorius MC5balance (the static settling for which is shown in FIG. 7) was used. Thepowder compounds and target dispense weights tested were Lidocaine (1mg), BSA (0.5 mg) and Agarose (0.25 mg). The table below shows theaverage weight actually dispensed (in mg) and the standard deviationfrom this average. The table also shows what minimum and maximum weightswere dispensed in a 50 sample experiment. As can be seen, the minimumand maximum values stray from the average value by about 0.05 mg orless. The standard deviation is 2 or 3% of the average indicating verygood dispense repeatability. The table also shows the time in secondsthat it took for the dispense to be achieved. This is typically around 8seconds for all the powder types. Interestingly, Agarose, which has beenfound to be difficult to dispense using traditional methods due to itspoor flowability was dispensed with a standard deviation of only 9 μg.However, the time taken to dispense Agarose is more varied showing astandard deviation of 15% of the average as compared to 8% for Lidocaineor BSA.

Lidocaine BSA Agarose Target Dose Wt. 1.00 mg 0.50 mg 0.25 mg Weight(mg) Time (s) Weight (mg) Time (s) Weight (mg) Time (s) Average 1.0187.975 0.503 8.148 0.252 7.790 Std. Dev. 0.026 0.637 0.012 0.643 0.0091.201 % CV 2.537 7.985 2.432 7.889 3.517 15.419 Minimum 0.944 6.6780.463 6.810 0.237 5.208 Median 1.022 8.002 0.506 8.269 0.251 7.876Maximum 1.062 9.445 0.528 9.323 0.276 10.313

1. Apparatus for dispensing particles, comprising: a particle retainerfor retaining a supply of the particles to be dispensed; a particlerelease actuator for causing, in response to an actuation signal, someof said supply of particles to be dispensed from said particle retainer;a weight measuring device for measuring the apparent weight of particlesdispensed from said particle retainer and for outputting a signalrepresenting the measured apparent weight; wherein said particle releaseactuator is arranged to transmit a discrete impulse of force to saidparticle retainer; and wherein the energy of said discrete impulse offorce corresponds to a characteristic of said actuation signal providedto said particle release actuator, whereby the number of particlesdispensed from said particle retainer is related to the energy of saiddiscrete impulse of force; further comprising a processor operativelyconnected to said particle release actuator and arranged to provide saidactuation signal thereto, said processor also being operativelyconnected to said weight measuring device and being arranged to receivesaid measured apparent weight signal therefrom; wherein said processorprovides an actuation signal having a characteristic that causes a lessenergetic discrete impulse of force to be transmitted to said particleretainer as the weight of particles dispensed approaches a targetweight.
 2. Apparatus according to claim 1,wherein said particle releaseactuator is spaced apart from said particle retainer by means of a rod.3. Apparatus according to claim 2,wherein said particle retainer andparticle release actuator are supported by a pivot and a spring so thatthe lower end of the particle retainer may be lifted out of, and loweredinto, a particle cassette cavity.
 4. Apparatus according to claim 1,wherein said particle release actuator is a solenoid.
 5. Apparatusaccording to claim 1, wherein said particle retainer comprises aplurality of apertures through which said particles are dispensed.
 6. Amethod of dispensing particles, said method comprising the steps of:retaining a supply of particles to be dispensed; providing an actuationsignal; transmitting a discrete impulse of force to said retained supplyof particles, wherein the energy of said discrete impulse of forcecorresponds to a characteristic of said actuation signal, to therebycause some of said supply of particles to be dispensed, wherein thenumber of particles dispensed is related to the energy of said discreteimpulse of force; and measuring the apparent weight of particlesdispensed and outputting a signal representing the measured apparentweight; wherein said discrete impulse of force has less energy as theweight of particles dispensed approaches a target weight.
 7. A methodaccording to claim 6, wherein said discrete impulse of force is providedby a horizontally disposed solenoid.
 8. A method according to claim 6,wherein said particles are dispensed through a plurality of apertures.9. Apparatus for dispensing particles, comprising: a particle retainerfor retaining a supply of the particles to be dispensed; a particlerelease actuator for causing, in response to an actuation signal, someof said supply of particles to be dispensed from said particle retainer;a weight measuring device for measuring the apparent weight of particlesdispensed fiom said particle retainer and for outputting a signalrepresenting the measured apparent weight; wherein said particle releaseactuator is arranged to transmit a discrete impulse of force to saidparticle retainer; and wherein the energy of said discrete impulse offorce corresponds to a characteristic of said actuation signal providedto said particle release actuator, whereby the number of particlesdispensed from said particle retainer is related to the energy of saiddiscrete impulse of force; further comprising a processor operativelyconnected to said particle release actuator and arranged to provide saidactuation signal thereto, said processor also being operativelyconnected to said weight measuring device and being arranged to receivesaid measured apparent weight signal therefrom; wherein said processorprovides an actuation signal having a characteristic that causes lessfrequent discrete impulses of force to be transmitted to said particleretainer as the weight of particles dispensed approaches a targetweight.
 10. Apparatus according to claim 9, wherein said particlerelease actuator is spaced apart from said particle retainer by means ofa rod.
 11. Apparatus according to claim 10, wherein said particleretainer and particle release actuator are supported by a pivot and aspring so that the lower end of the particle retainer may be lifted outof, and lowered into, a particle cassette cavity.
 12. Apparatusaccording to claim 9, wherein said particle release actuator is asolenoid.
 13. Apparatus according to claim 9, wherein said particleretainer comprises a plurality of apertures through which said particlesare dispensed.
 14. A method of dispensing particles, said methodcomprising the steps of: retaining a supply of particles to bedispensed; providing an actuation signal; transmitting a discreteimpulse of force to said retained supply of particles, wherein theenergy of said discrete impulse of force corresponds to a characteristicof said actuation signal, to thereby cause some of said supply ofparticles to be dispensed, wherein the number of particles dispensed isrelated to the energy of said discrete impulse of force; and measuringthe apparent weight of particles dispensed and outputting a signalrepresenting the measured apparent weight; wherein said discrete impulseof force is less frequent as the weight of particles dispensedapproaches a target weight.
 15. A method according to claim 14, whereinsaid discrete impulse of force is provided by a horizontally disposedsolenoid.
 16. A method according to claim 14, wherein said particles aredispensed through a plurality of apertures.